Orientadores: Alex Antonelli, Maurice de Koning / Dissertação (mestrado) - Universidade Estadual de Campinas, Instituto de Física Gleb Wataghin / Made available in DSpace on 2018-08-18T18:03:40Z (GMT). No. of bitstreams: 1 CajahuaringaMacollunco_OscarSamuel_M.pdf: 6673580 bytes, checksum: a344f89389b318a79fb73ef903615a6b (MD5) Previous issue date: 2011 / Resumo: A física dos líquidos super-resfriados é um dos problemas para o qual ainda não existe uma única teoria que tenha capturado com sucesso todas as características destes materiais, principalmente a origem da dinâmica complexa, e também a possível ocorrência de transições líquido-líquido nesse regime. Nosso trabalho está focado nas propriedades dinâmicas do gálio, que é evidenciada pelas funções de correlação temporais antes e depois da transição de fase líquido-líquido. Primeiro, foram feitas simulações atomísticas no gálio através de dinâmica molecular usando o modied embedded atom model (MEAM) e condições periódicas de contorno em uma super-célula contendo 1152 átomos, com o propósito de mostrar a transição de fase líquido-líquido obtida em recentes pesquisas teóricas. Para estudar a dinâmica do sistema como um todo, calculamos o deslocamento quadrático médio, que revela o platô em tempos intermediários, o qual se torna mais notório após a transição líquido-líquido. Esse comportamento pode ser originado por uma dinâmica espacialmente homogênea ou uma dinâmica espacialmente heterogênea. Para saber qual das duas hipóteses é mais relevante foi medido o parâmetro não-gaussiano de ordem 2, porque este nos fornece informação do grau de heterogeneidade dinâmica do sistema, e que mostrou que nosso sistema possui uma dinâmica heterogênea. Posteriormente, foi calculada a auto-função intermediária de espalhamento usando o método da transformada rápida de Fourier que é mas eciente para tempos de correlação longos. Esta função fornece a correlação na densidade de partículas no espaço recíproco, que mostra também um platô em tempos intermediários. Com o fim de analisar como relaxa cada partícula, baseados na ideia da dinâmica espacialmente heterogênea, foi possível separar as partículas pela sua dinâmica em dois grupos, um grupo que possui a dinâmica mais difusiva e outro que possui a dinâmica menos difusiva. Finalmente, foram caracterizados estruturalmente esses dois grupos e, comparando-os com as funções estruturais do sistema todo, concluímos que as duas fases presentes no líquido depois da transição, o líquido de alta densidade possui uma dinâmica mais difusiva e o líquido de baixa densidade possui uma dinâmica menos difusiva. Foi possível com estes resultados identicar espacialmente as duas fases líquidas e observar claramente os seus próprios domínios e que estes não estão misturados / Abstract: The physics of supercooled liquids still lacks a single theory which can successfully capture all features of these materials, mainly the cause for their complex dynamics and the possibility of liquid-liquid phase transitions in this regime. Our work is focused on the dynamics of liquid gallium, which was investigated through the correlation functions before and after the liquid-liquid phase transition. First, atomistic simulations were performed using the modied embedded atom model (MEAM) and periodical boundary conditions in a 1152-atom supercell, in order to obtain the liquid-liquid phase transition observed in recent previous simulations. To study the dynamics of the whole system, we calculate the mean square displacement, which shows the plateau for intermediate times that becomes much more noticeable after the liquidliquid transition. This behavior can be caused by either a spatially homogeneous dynamics or a spatially heterogeneous dynamics. In order to find out which hypothesis is more relevant for our case, the second order non-Gaussian parameter was determined, since it provides the degree of heterogeneity of the dynamics of the system, showing that system exhibits a heterogeneous dynamics. Later, the self-intermediate scattering function was calculated using the fast Fourier transform method, which is more ecient for long correlation times. This function gives the density particle correlation in reciprocal space, showing a plateau in intermediate times as well. In order to analyze how each particle relaxes, based on the idea of a spatially heterogeneous dynamics, it was possible to gather the particles according to their mobility in two groups, one which has a more diffuse dynamics and another which has a less diffuse dynamics. Finally, these two groups were structurally characterized and by comparing them with the structural functions of the whole system, it was possible to determine that the liquid of higher density has a more diffusive dynamics, whereas the lower density liquid has less diffusive dynamics. From these results we were able to spatially identify the two liquid phases, which clearly display their own domains that do not mix with each other / Mestrado / Física da Matéria Condensada / Mestre em Física

Orientador: Alex Antonelli / Tese (doutorado) - Universidade Estadual de Campinas, Instituto de Física Gleb Wataghin / Made available in DSpace on 2018-08-29T05:01:21Z (GMT). No. of bitstreams: 1 CajahuaringaMacollunco_OscarSamuel_D.pdf: 15985103 bytes, checksum: f54d17d6335170c62196c9e329f257d9 (MD5) Previous issue date: 2015 / Resumo: Apesar de serem substâncias muito diferentes, silício e gálio, na fase líquida, compartilham muitas anomalias nas suas propriedades termodinâmicas. Evidências teóricas e experimentais sugerem que esses líquidos podem sofrer a chamada transição de fase líquido-líquido (LLPT). Especula-se que este tipo de transição é acompanhada por uma transição dinâmica entre um líquido frágil e um líquido forte, com base nas hipóteses de que o surgimento de um "dip" na função auto-intermediária de espalhamento logo após o regime balístico e o aparecimento do excesso de modos vibracionais em baixas frequências após a LLPT estariam relacionados com o comportamento de líquidos fortes. Foi realizado um estudo da dinâmica desses sistemas através das funções de correlação nas vizinhanças da LLPT usando simulações clássicas. Observamos apenas no caso do silício o aparecimento do "dip" na função auto-intermediária de espalhamento. A densidade de estados vibracionais reduzida de ambos os líquidos apresenta picos em baixas frequências, sugerindo que ambos os líquidos seriam fortes. Desta forma, nos dois casos estudados, as duas hipóteses não são conclusivas. Visando um melhor entendimento, determinamos a viscosidade de cisalhamento de ambos os líquidos em um amplo intervalo de temperatura. A apresentação desses resultados no chamado gráfico de Angell, indica que, em ambos os casos, a LLPT é acompanhada de uma transição de um líquido frágil para um líquido menos frágil, o que não dá suporte às especulações de uma transição frágil-forte. Além de investigar a LLPT em gálio "bulk", foi também estudado o gálio líquido confinado em nanofendas, ou seja, um sistema quase-bidimensional. Foi observada a transição de fase de primeira ordem entre um líquido isotrópico e um líquido ordenado. Por meio de uma série de análises estruturais, tanto de ordem translacional quanto orientacional, conseguimos identificar o líquido ordenado como a fase hexática, que é prevista ocorrer em sistemas bidimensionais segundo a teoria de Kosterlitz-Thouless-Halperin-Nelson-Young (KTHNY). Como a LLPT em gálio bulk foi identificada em simulações de dinâmica clássica, realizamos um estudo visando obter evidência da LLPT em simulações de primeiros princípios, que são em princípio mais realísticas. Utilizando o chamado método-Z, que permite estimar a temperatura de fusão, determinamos que o regime super-resfriado do gálio líquido descrito por cálculos de primeiros princípios ocorre em temperaturas abaixo de 400 K. Partindo de um líquido em equilíbrio em 500 K, realizamos simulações a pressão constante igual a zero em que o líquido foi resfriado para 260 K em um intervalo de 145 ps. Não foi observada uma mudança abrupta no volume durante o resfriamento. A fim de melhorar a amostragem em nossas simulações de primeiros princípios, realizamos um estudo de dinâmica molecular a volume constante com troca de réplicas. Foram usadas um total de 10 réplicas entre 400 K e 260 K, em simulações com a duração de 100 ps. Neste caso, a pressão decresceu monotonicamente com a temperatura, o que é característico de líquidos simples que não sofrem LLPT. Cabe ressaltar que nas simulações clássicas que identificaram a LLPT em gálio, a taxa de resfriamento foi muito mais lenta, da ordem de nano-segundos, que seria inexequível para simulações de primeiros princípios / Abstract: Despite of being very different substances, silicon and gallium, in their liquid phase, share several anomalous thermodynamic properties. Theoretical and experimental evidence suggest that these liquids can undergo the so-called liquid-liquid phase transition (LLPT). There has been speculated that this transition is accompanied by a dynamic transition form a fragile liquid to a strong liquid, based on the hypothesis that the development of a dip in the self-intermediate scattering function, just after the ballistic regime, and the appearance of excess low frequency vibrational modes just after the LLPT would be related to the behavior of strong liquids. It was performed a study of the dynamics of these systems through the correlation functions in the vicinity of the LLPT using classical simulations. We observed the development of a dip in the self-intermediate scattering function only in the case o silicon. The reduced density of vibrational states of both liquids exhibits peaks in low frequencies, suggesting both liquids to be strong. Therefore, for the two cases we studied, the two hypotheses are not conclusive. In order to achieve a better understanding, we determined the shear viscosity of both liquids for a wide range of temperatures. By plotting the data in the so-called Angell plot one can see that, in both cases, the LLPT is accompanied by a transition of a fragile liquid to a less fragile liquid, which does not give support to the speculations of a fragile-to-strong transition. Aside from investigating the LLPT in bulk gallium, it was also studied liquid gallium confined in nanoslits. i.e., a quasi two-dimensional system. It was observed a first-order transition between an isotropic liquid and an ordered liquid. Through a series of structural analyses, both translational and orientational, we were able to identify the ordered liquid as the hexatic phase, which is predict to occur in two-dimensional systems according to the Kosterlitz-Thouless-Halperin-Nelson-Young (KTHNY) theory. Since the LLPT in gallium has been found in classical molecular dynamics simulations, we performed a study aimed to obtain evidence of the LLPT in first-principles simulations, which are, in principle, more realistic. Using the so-called Z-method, which allows one to estimate the melting temperature, we determined the supercooled regime of liquid gallium, described by first-principles, to occur below 400 K. Starting from an equilibrated liquid at 500 K, we performed simulations at zero pressure in which the liquid was cooled down to 260 K in an interval of 145 ps. No abrupt change in the volume was observed as the liquid was cooled. In order to improve sampling in our first-principles simulations, we performed a study using constant volume molecular dynamics with replica exchange. Ten replicas were used between 400 K and 260 K, in simulations 100 ps long. In this case, pressure decreased monotonically with temperature, which is the behavior of simple liquids, which do not exhibit the LLPT. It should be emphasized that in the classical simulations that identified the LLPT in gallium, the cooling rates were much slower, of the order of nanoseconds, which would be unfeasible for first-principles simulations / Doutorado / Física / Doutor em Ciências / 1000949 / CAPES

Este trabalho fundamentou-se na concepção, desenvolvimento tecnológico, ampliação de escala e avaliação do comportamento de sistema combinado anaeróbio-aeróbio de leito fixo e fluxo ascendente, com recirculação da fase líquida, para tratamento de esgoto sanitário. O reator, em escala piloto, foi construído em formato cilíndrico e confeccionado em fibra de vidro com volume total de aproximadamente 2,5 \'M POT.3\', com intuito de desenvolver um sistema capaz de operar como única unidade de tratamento para remoção de matéria orgânica e nitrogênio, reduzindo a geração de lodo e o consumo de energia pela combinação dos processos anaeróbio e aeróbio, possibilitando o aproveitamento das vantagens de cada um e minimizando seus aspectos negativos. Os melhores resultados operacionais foram encontrados para a etapa com tempo de detenção hidráulica total (TDH) de 12 horas e razão de recirculação (r) igual a 3,0, apresentando eficiências médias de remoção de DQO, \'N\'-NTK e SST de 92 ± 3%; 68 ± 11% e 75 ± 7%, respectivamente, com valores médios efluentes de 54 ± 22 mgDQO/L, 14 ± 10 mg \'N\'-NTK/L e 70 ± 42 mgSST/L. Os valores médios de carga orgânica volumétrica (COV) e carga volumétrica de nitrogênio (CVN) removidas foram de 1,08 ± 0,04 kgDQO/\'M POT.3\'.dia e 0,06 ± 0,02 kgNTK/\'M POT.3\'.dia para esta etapa. A estabilidade operacional durante a etapa com TDH de 12 h, a alta remoção de matéria orgânica e nitrogênio, sem a necessidade de adição de fonte exógena de carbono, para promover o processo de desnitrificação, e de suplementação de alcalinidade consumida durante a nitrificação, e a reduzida necessidade de manutenção devido à tecnologia de fabricação adotada, comprovam a viabilidade técnica de utilização do reator combinado de leito fixo como unidade compacta para pequenas comunidades ou vazões afluentes, para tratamento de esgoto sanitário. / This work was based on design, technology development, scale up and performance evaluation of an up-flow combined anaerobic-aerobic fixed bed system, with recycle of the liquid phase, for treatment of domestic sewage. The pilot scale reactor was built in a fiberglass cylindrical shape with a total volume of approximately 2.5 \'M POT.3\', aiming at the development of a system capable of operate as a single treatment unit for organic matter and nitrogen removal, with low sludge production and energy consumption by the advantages of combination of anaerobic and aerobic processes. The improved operating results were found for the condition with overall hydraulic retention time (HRT) of 12 hours and recycle ratio (r) equal to 3.0, with average removal efficiencies of COD, TKN and TSS of 92 ± 3%, 68 ± 11% and 75 ± 7%, respectively, with average effluent values of 54 ± 22 mgCOD/L, 14 ± 10 mgTKN/L and 70 ± 42 mgTSS/L. The average values of removed organic loading rate (OLR) and nitrogen volumetric loading (NVL) reached 1.06 ± 0.04 kgCOD/\'M POT.3.d and 0.06 ± 0.02 kgTKN/\'\'M POT.3\'.d for this phase. The operational stability during the stage with HRT of 12 h, the high organic matter and nitrogen removal, without addition of exogenous carbon source (electron donor) to promote the denitrification process, with no supplementation of alkalinity consumed during nitrification, and the reduced maintenance due to manufacturing technology adopted, proved the technical feasibility of the combined fixed-bed reactor as a compact unit for small communities or low inflow rates, for treatment of domestic sewage.

How do fuel and air mix, if a liquid fuel is injected into an environment featuring pressure and temperature that exceed the critical pressure and the critical temperature of the fuel? It is subject of current discussion on whether and if so when, the fuel/air-mixture becomes supercritical or not. We here report experimental data comprising three mixture properties that are relevant for the current debate, all spatially and temporally resolved throughout the spray and injection event: The overall composition of the fuel/air-mixture, the liquid fraction of the fuel/air-mixture, and the temperature of the liquid phase. To this end, we applied Raman spectroscopy and gave special attention to the signature of the Raman OH-band of ethanol, which we used as fuel. Its signature is connected to the development of a hydrogen bonded network between the ethanol molecules and thus extremely sensitive to thermodynamic state and temperature. Measurements were carried out in a high-pressure, high-temperature combustion vessel in a pressure range of 3−8 MPa and a temperature range of 573−923 K. For the highest set temperature we found ethanol in liquid-like mixtures that exceeded the mixture critical temperature. This is an indication of the existence of a single-phase mixing path.

Grafen v kombinaci s komplexy kovů by mohl poskytnout nové přísutpy v hybridních materiálech založených na grafenové bázi a v oblasti molekulárního magnetismu. Obě témata jsou velmi diskutovaná jako taková, nicméně, výzkumu vedoucího k možnosti jejich míchání není mnoho. Vzorky byly připraveny sonikací grafitu v kapalné fázi, což vedlo k exfoliaci grafenu. Následně byly nadeponovány pomocí modiikované Lagmuirovy– Schaeferovy depoziční metody různé komplexy kovů na substrát pokrytý grafenem. Klíčovým krokem bylo určení vlastností takto připraveného materiálu. Proto byly následně vlastnosti takového hybridního materiálu charakterizovány pomocí vysokofrekvenční elektronové paramagnetické rezonance (angl. HFEPR), rastrovacího elektronového mikroskopu, (angl. SEM), Ramanovou spektroskopií a čtyř bodovou metodou měření odporu. V této práci jsme potvrdili naši presumpci, že je možné vytvořit hybridní materiál smícháním exfoliovaného grafenu s molekulárními magnety pro získání nových magnetických a elektronických vlastností, které by mohly být využity v další generaci detektorů a elektroniky.

Liquid composition for antimony doped tin oxide solgel deposition was prepared. Anorganic precursors of tin and antimony were used (tin(IV) chloride, antimony(III) chloride). ATO nanoparticles were dispergated in composition. This composition was used for spincoating deposition of thin films. Composition was analyzed by thermal analysis TGA and DSC. Sheet resistence of prepared samples were examined by four probe sensing. RMS roughness and thickness was measured by profilometry. Samples were analyzed by scan electron microscopy (SEM), X-ray diffraction (XRD) and X-ray photoelectron spectroscopy (XPS). Transmittance and haze were measured and calculated by UV-VIS spektrometry with integration sphere.

Les oxydes de métaux de transition lamellaires peuvent servir de catalyseurs pour la conversion de la biomasse, mais leur développement nécessite une meilleure compréhension de leurs propriétés. En conséquence, plusieurs matériaux lamellaires, tels que HNbMoO6, HNbWO6, H2W2O7 et H2WO4, ainsi qu'un nouveau type d'oxydes en couches basés sur Nb et W et caractérisés par des phases d'Aurivillius “en escalier” ont été largement caractérisés notamment par spectroscopie DRX et spectroscopie Raman. La possibilité de convertir les solides précurseurs au lithium ou bismuth en phases protonées a été étudiée. Ces oxydes ont la spécificité d'intercaler des molécules entre les couches, ce qui peut contribuer à l’activité catalytique en phase liquide. Pour identifier les rôles respectifs de l’intercalation et des propriétés de surface comme l’acidité, les matériaux ont été caractérisés en phase liquide par spectroscopie Raman en utilisant des bases organiques telles que les n-alkylamines (butylamine et octylamine) et la pyridine. L'intercalation avec des réactifs possibles, les n-alcools et le 2,5-hexanediol, a également été étudiée. L'activité catalytique de ces oxydes lamellaires a été déterminée grâce à une nouvelle réaction: la cyclo-déshdrataion du 2,5-hexanediol en 2,5-diméthyltétrahydrofurane. HNbMoO6 s’est avéré le catalyseur le plus actif, comparé à des catalyseurs acides conventionnels ou aux autres matériaux lamellaires. L’acidité et la capacité d’intercalation de ces divers matériaux lamellaires ont été comparées pour comprendre les différences observées pour l’activité catalytique. / Layered transition metal oxides have a potential as catalysts for biomass conversions, but their development necessitates a better understanding of their properties. Consequently, several layered materials such as HNbMoO6, HNbWO6, H2W2O7 and H2WO4 as well as new types of layered oxides based on Nb and W and characterized by a “stair-like” Aurivillius phases were extensively characterized notably by XRD and Raman spectroscopy. The possibility to convert the as-synthesised lithium or bismuth precursors to protonated phases was also thoroughly evaluated. Layered oxides have the specificity to intercalate molecules within their interlayer regions, which may be a key feature to catalytic activity for reactions in the liquid phase. In order to evaluate the respective roles of intercalation and surface properties such as acidity, the materials were characterized in the liquid phase by Raman spectroscopy using organic bases such as n-alkylamines (butylamine and octylamine) and pyridine. Intercalation with possible reagents, n-alcohols and 2,5-hexanediol, was also studied. The catalytic activity of these layered oxides was evaluated using a novel test reaction: the cyclo-dehydration of 2,5-hexanediol into 2,5-dimethyltetrahydrofuran. HNbMoO6 proved to be the most active catalyst, compared to conventional acidic catalysts or other layered materials. The acidity and intercalation ability of the various layered materials were compared to understand the differences observed for the catalytic activity.

Zellen sind in der Lage, gleichzeitig ganz unterschiedliche biochemische Prozesse zu bewältigen. Dies gelingt ihnen durch eine Einteilung ihres Inneren in Kompartiemente, sogennante Organellen, die die jeweils geeignete biochemische Umgebung für die unterschiedlichen Aufgaben schaffen. Bei membranumschlossenen Kompartimenten ist leicht vorstellbar, dass sie eine andere biochemische Zusammensetzung als ihre Umgebung haben können. Jedoch existieren auch Organelle ohne Membran die durch eine flüssig-flüssig Phasenseparation entstehen. Manche dieser Kompartiemente haben die Fähigkeit, RNA zu binden und Proteinkomplexe auszubilden, während andere auf die Veränderungen innerhalb der Zelle, wie z.B. die Veränderung des pH-Werts und der damit Verbunden Änderung ihres Protonierungszustands, reagieren können. Um diese Prozesse theoretisch analysieren zu können, entwickeln wir zunächst ein allgemeingültiges, thermodynamisches Gerüst, um Systeme zu untersuchen, die im chemischen Gleichgewicht flüssig-flüssig hasensepariert vorliegen können. Dies erlaubt, basierend auf den Erhaltungsgrößen, im chemischen Gleichgewicht thermodynamisch konjungierten Variablen zu identifizieren, welche aus den erhaltenen Komponenten und den zugehörigen chemischen Potentialen bestehen. Mithilfe des obig erwähnten Gerüsts können wir den Einfluss des pH-Wertes auf die flüssig-flüssig Phasenseparation in einem minimalen Modell untersuchen. Dies beschreibt die makromolekulare Phasenseparation, kontrolliert durch Protonierungs- und Deprotonierungreaktionen, welche wiederum vom pH-Wert abhängig sind. Unsere Untersuchung der pH-Abhängigkeit der Phasenseparation kommt zu folgenden Ergebnissen: Erstens liegt die größte Region von Phasenseparation im Phasendiagramm typischerweise im Bereich des isoelektrischen Punkts. Zweitens zeigt das Modell eine Fähigkeit der erneuten Mischung auf. Drittens ist die Topologie des Phasendiagrams von der dominantesten Interaktion bestimmt. Unser Modell stimmt mit experimentellen Beobachtungen zur Phasenseparation von intrinsisch ungeordneten, Proteinen, deren Struktur sich pH abhängig verändern, überein. Das Modell ist außerdem konsistent mit Beobachtungen von Phasenseparation von Proteinen im Zytosol von Hefezellen, die entsteht, wenn der intrazellulare pH-Wert in die Nähe des isoelektrischen Punkt dieser Proteine gebracht wird. Des Weiteren geht diese Arbeit auf den physikalischen Mechanismus ein, mit dem flüssigkeitsähnliche Organellen, sog. P granules, im Organismus Caenorhabditis elegans positioniert werden. Um dieses Phänomen zu analysieren, stellen wir zunächst experimentelle Beobachtungen vor, die zeigen, dass PGL-3, eine Hauptkomponente der P granules, flüssigkeitsähnliche Tropfen bildet, deren Zusammensetzung von RNA moduliert werden kann. Darüber hinaus zeigen wir Daten, die großen Unterschiede zwischen der RNA-Bindungsaffinität von Proteinen wie Mex-5, die für die Positionierung der P granules relevant sind, und solchen, die P granules bilden, wie PGL-3, zeigen. Dies deutet darauf hin, dass eine Konkurrenz zwischen den Bestandteilen der P Granula und MEX-5 um die zur Bindung zur Verfügung stehende RNA besteht, die die Kondensation und Auflösung von P Granula räumlich kontrollieren könnte. Auf diesen experimentellen Befunden aufbauend führen wir ein minimalles Modell ein, in dem wir die Phasenseparation von PGL-3 an Bindungsreaktionen der MEX-5 Proteine und RNA koppeln. Um die experimentellen Beobachtungen beschreiben zu können, muss die Neigung des PGL-3 Proteins zur Phasenseparation zunehmen, wenn es Komplexe mit RNA bildet. Dies unterstützt die Idee, dass MEX-5 diese Phasenseparation unterdrückt, indem es die Anzahl an möglichen RNA-Bindungspartner für PGL-3 herabsetzt und damit die weitere Entstehung derartiger Protein-RNA-Komplexe erschwert. Dieser einfache Mechanismus scheint die Hauptursache dafür zu sein, dass P granules auf der posterioren Seite des Caenorhabditis elegans Embryos zu finden sind. / One of the main features of cells is their incredible ability to control biochemical processes in space and time. They do so by organizing their interior in sub-compartments called organelles, each of them with a different biochemical environment that allows them to perform specific tasks in the cell. It is sometimes believed that these compartments need a membrane in order to have a stable biochemical environment and regulat their compositions. However, there are some organelles which lack a membrane and seem to form and organize via liquid-liquid phase separation. Some of the components that form these membraneless organelles have the ability to bind to RNA and form complexes, while some others react to changes in the intracellular environment such as pH variations, which in turn affects their protonation state. In order to study these processes from a theoretical perspective, we develop a generic thermodynamic framework to study systems exhibiting liquid-liquid phase separation at chemical equilibrium. This framework, based on the use of conservation laws in chemical reactions, allow us to identify thermodynamic conjugate variables at chemical equilibrium, which are given by a set of conserved quantities and the corresponding conjugate chemical potentials. Within the aforementioned framework, we introduce a minimal model to study the effect of pH on liquid-liquid phase separation. Our model explains macromolecular phase separation controlled by protonation and deprotonation reactions, which are tuned by the pH of the system. We study the phase behavior of the system as a function of pH. Our main findings are: Firstly, the broadest region of phase separation is typically found at the isoelectric point. Secondly, the system exhibits reentrant behavior. Thirdly, that the dominating interaction in the system determines the topology of the phase diagrams. Our model is in agreement with experimental observations of in vitro protein phase separation of pH-responsive intrinsically disordered proteins, as well as with observations of protein phase separation exhibited by many cytosolic proteins when the intracellular pH in yeast cells is brought close to the isoelectric point of such proteins. Moreover, this work analyses the physical mechanism behind the positioning of liquid-like organelles in the {\it{Caenorhabditis elegans}} organism known as P granules. In order to study this phenomenon, we first present firm experimental evidence showing that PGL-3 protein, a key component of P granules, forms liquid-like drops whose assembly can be modulated by RNA. We then present data showing that the RNA-binding affinity differs significantly between proteins relevant for the positioning of P granules, such as MEX-5 and the proteins forming the P granules, like the aforementioned PGL-3. This points to a possible mechanism of RNA-binding competition between P granule constituents and MEX-5 in order to spatially control the condensation and dissolution of P granules. Based on the experimental evidence, we propose a minimal model in which we couple phase separation of PGL-3 to a set of binding reactions involving the MEX-5 protein and RNA. We find that in order to explain the experimental data, the tendency for phase separation of the PGL-3 protein increases with the formation of complexes of PGL-3 bound to RNA. This therefore supports the idea that MEX-5 inhibits this protein phase separation by depleting the RNA available for PGL-3 to form such complexes. This simple mechanism is at the core of how P granules localize to the posterior side of the Caenorhabditis elegans embryo.

In der vorliegenden Arbeit wurde die Verwendung der kostengünstigen aber sauerstoffaffinen Legierungselemente Mangan, Silizium und Chrom in pulvermetallurgisch hergestellten Sinterstählen untersucht. Das Einbringen der Legierungselemente erfolgte mit Hilfe unterschiedlicher Masteralloysysteme. In der vorliegenden Arbeit wurden insgesamt 18 chemisch unterschiedliche, niedriglegierte Sinterstähle entwickelt und untersucht.

Over the past decade, the bottom-up synthesis of structurally defined graphene nanoribbons (GNRs) with various topologies has attracted significant attention due to the extraordinary optical, electronic, and magnetic properties of GNRs, rendering them suitable for a wide range of potential applications (e.g., nanoelectronics, spintronics, photodetectors, and hydrothermal conversion). Remarkable achievements have been made in GNR synthesis with tunable widths, edge structures, and tailor-made functional substitutions. In particular, GNRs with liquid-phase dispersibility have been achieved through the decoration of various functional substituents at the edges, providing opportunities for revealing unknown GNR physiochemical properties. Because of the promise of liquid-phase dispersible GNRs, this mini-review highlights recent advances in their synthetic strategies, physiochemical properties, and potential applications. In particular, deep insights into the dvantages and challenges of their syntheses and chemical methodologies are provided to encourage future endeavors and developments.